Method and device for the generation of a plasma through electric discharge in a discharge space
View Patent ↗The invention relates to a method and a device for the generation of a plasma through electric discharge in a discharge space which contains at least two electrodes, at least one of which is constructed from a matrix material or carrier material, such that an erosion-susceptible region with an evaporation spot is formed at least by the current flow. To present a method or a device for the generation of a plasma by electric discharge, it is suggested that a sacrificial substrate ( 38 ) is provided at least at the evaporation spot, the boiling point of said sacrificial suvstrate (38) during discharge operation lying below the melting point of the carrier material ( 30 ), such that charge carriers arising in the current flow are mainly generated from the sacrificial substrate ( 38 ).
1. A method for the generation of a plasma through electric discharge in a discharge space which contains at least two electrodes, at least one of which is constructed from a matrix material or carrier material, such that an erosion-susceptible region with an evaporation spot is formed at least by the current flow, characterized in that a sacrificial substrate ( 38 ) is provided at least at the evaporation spot, the boiling point of said sacrificial substrate ( 38 ) during discharge operation lying below the melting point of the carrier material ( 30 ), such that charge carriers arising in the current flow are mainly generated from the sacrificial substrate ( 38 ).
2. A method as claimed in claim 1 , characterized in that the sacrificial substrate ( 38 ) is supplied through the electrode ( 10 ) to a surface ( 36 ) that faces the electric discharge.
3. A method as claimed in claim 1 , characterized in that said surface ( 36 ) is wetted by the sacrificial substrate ( 38 ).
4. A method as claimed in claim 1 , characterized in that the discharge is operated at an average temperature (T) of the electrodes ( 10 ) that lies above the melting point of the sacrificial substrate ( 38 ).
5. A method as claimed in claim 1 , characterized in that the mass of the sacrificial substrate ( 38 ) evaporated by the discharge is supplemented from a reservoir ( 34 ).
6. A method as claimed in claim 1 , characterized in that the evaporated sacrificial substrate ( 38 ) is returned into a or the reservoir ( 34 ) after condensation.
7. A method as claimed in claim 1 , characterized in that the electric discharge is operated on the left-hand branch of the Paschen curve at a given gas pressure (p).
8. A method as claimed in claim 1 , characterized in that a gas is present between the electrodes ( 10 , 12 ), which gas comprises at least one component that generates radiation ( 28 ).
9. A method as claimed in claim 8 , characterized in that a main ingredient of the gas is transparent to the emitted radiation ( 28 ).
10. A method as claimed in claim 1 , characterized in that substantially more sacrificial substrate is evaporated through a short-period introduction of additional energy before the discharge at least in that location or those locations where the cathode spots or evaporation areas usually occur, for example by means of a laser pulse or electron beam.
11. A method as claimed in claim 1 , characterized in that sacrificial substrates ( 38 ) such as tin, indium, gallium, lithium, gold, lanthanum, aluminum, and alloys thereof and/or chemical compounds thereof with other elements are used.
12. A device for generating a plasma through electric discharge, comprising a discharge space ( 22 ) having at least two electrodes, of which at least one is constructed from a matrix material or carrier material such that an erosion-susceptible region with an evaporation spot is formed at least owing to the flow of current, characterized by an arrangement which supplies a sacrificial substrate ( 38 ) at least at the evaporation spot, the boiling point of said sacrificial substrate ( 38 ) lying below the melting point of the carrier material ( 30 ) during discharge operation, such that charge carriers arising in the case of a flow of current can be generated mainly from the sacrificial substrate ( 38 ).
13. A device as claimed in claim 12 , characterized in that a plasma ( 26 ) can be formed along an axis of symmetry ( 24 ) defined by openings ( 14 , 16 ) in the discharge space, which is formed by at least two electrodes ( 10 , 12 ) and at least one insulator ( 18 ), when a defined ignition voltage is reached.
14. A device as claimed in claim 12 , characterized in that the carrier material ( 30 ) is porous or has capillary-type channels ( 48 ).
15. A device as claimed in claim 12 , characterized in that the carrier material ( 30 ) is connected to at least one reservoir ( 34 ) which contains the sacrificial substrate ( 38 ) in liquid and/or gaseous form.
16. A device as claimed in claim 12 , characterized in that the carrier material ( 30 ) is formed by a refractive material, preferably a metal or a metal alloy, or from a ceramic material.
17. A device as claimed in claim 12 , characterized in that the carrier material ( 30 ) has a porous shape on at least one of the plasma-facing surfaces of one of the electrodes ( 10 ), which shape is different from the porous shape of other portions of the carrier material ( 30 ).
18. The use of the method and/or the device for the generation of plasma as claimed in claim 1 for the generation of radiation in the range of extreme ultraviolet and/or soft X-ray radiation, in particular for EUV lithography.
19. The use of the method and/or the device for the generation of plasma ( 26 ) as claimed in claim 1 for controlling very high current strengths, in particular for high-power switches.